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Modeling the Input Optics with e2e T. Findley, S. Yoshida, D. Dubois, N. Jamal, and R. Dodda Southeastern Louisiana University LIGO-G050219-00-D

Modeling the Input Optics with e2e

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Modeling the Input Optics with e2e. T. Findley, S. Yoshida, D. Dubois, N. Jamal, and R. Dodda Southeastern Louisiana University. LIGO-G050219-00-D. Objectives. Report status of e2e modeling Results Calibrated floor motion Better Mode Cleaner Mode Matching Telescope in Detector.box - PowerPoint PPT Presentation

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Page 1: Modeling the Input Optics with e2e

Modeling the Input Optics with e2e

T. Findley, S. Yoshida, D. Dubois, N. Jamal, and R. Dodda

Southeastern Louisiana University

LIGO-G050219-00-D

Page 2: Modeling the Input Optics with e2e

Objectives

Report status of e2e modeling Results

Calibrated floor motion Better Mode Cleaner Mode Matching Telescope in Detector.box

Comments/Suggestions

Page 3: Modeling the Input Optics with e2e

Contents Estimate the table top motion for a given ground

motion. Make a Small Optic Suspension (SOS) box with

local damping, and find optimal gain settings to damp the optic when estimated table top motion is given.

Create a Mode Cleaner (MC) box, and implement the length control for the mode cleaner cavity.

Put all the optics (MCs, SM, and MMTs) in order, and create the Input Optic (IO) box.

Use the IO box in Simligo, and run the simulation for the entire detector.

Page 4: Modeling the Input Optics with e2e

Input Optics

Page 5: Modeling the Input Optics with e2e

Table Motion

HAM table

Vibration

isolation

stacks

Accelerometer

Suspension Point

Tower

Wire

OSEM Sensors

dtdtACCXtx )(

Page 6: Modeling the Input Optics with e2e

HAM box

Calibrating the Table Motion

MC1 box

Page 7: Modeling the Input Optics with e2e

ITMX pend/yaw with balanced OSEMs

Pendular Yaw

Page 8: Modeling the Input Optics with e2e

OSEM sensor imbalance

UL

LL

UR

LR

UR= (P + Y + T) g1

UL= (P - Y + T) g2

LL= (P - Y - T) g3

LR= (P + Y - T) g4

OSEM P = UR+UL+LL+LR = (P+Y+T)g1 + (P-Y+T) g2 + (P-Y-T) g3 + (P +Y-T) g4

=(g1+g2+g3+g4)P + (g1-g2-g3+g4)Y + (g1+g2-g3-g4)T

OSEM Y = UR–UL–LL+LR = 0.1P+3.9Y+0.1T

= 0, if g1=g2=g3=g4 If g1=1.05, g2=g3=g4=0.95

Page 9: Modeling the Input Optics with e2e

ITMX pend/yaw with pend/yaw ratio = 0.023

Pendular Yaw

Page 10: Modeling the Input Optics with e2e

Mode Cleaner

Page 11: Modeling the Input Optics with e2e

Mode Cleaner Continued

Page 12: Modeling the Input Optics with e2e

MC Transmission and MC2 motion

Page 13: Modeling the Input Optics with e2e

MC Transmitted Power

DAQE2E

Frequency Domain

Time Domain

Page 14: Modeling the Input Optics with e2e

MC Beam Motion

Beam center 20 meters away from MC pitch (lower)

Time Domain

Frequency Domain

yaw

pitc

h

Page 15: Modeling the Input Optics with e2e

Detector box

Page 16: Modeling the Input Optics with e2e

Status of IO box: Contains MMT optics only

Page 17: Modeling the Input Optics with e2e

MMT1 motion effect on CARM and DARM error signals

Time (sec)

Time (sec)

Dis

pla

cem

ent

(m o

r ra

d)

Page 18: Modeling the Input Optics with e2e

MMT3 motion effect on CARM and DARM

Time (sec)

Dis

pla

cem

ent

(m o

r ra

d)

Time (sec)

Page 19: Modeling the Input Optics with e2e

Power Behind ETMx due to MMT1 and MMT3 motion

Page 20: Modeling the Input Optics with e2e

Power Behind ETMx due to MMT optics motion

Page 21: Modeling the Input Optics with e2e

Summary

Produced a better representation of the table translational and yaw motion

Created a Mode Cleaner box with Length Sensing Control

Put the Mode Matching Telescope into Detector box

Will continue investigating the effect of table motion on the optic and the resultant beam motion

Will include Mode Cleaner box in Detector box

Page 22: Modeling the Input Optics with e2e

Acknowledgements

People: B. Bhawal M. Evans H. Yamamoto

Organizations LIGO Livingston Observatory National Science Foundation Southeastern Louisiana University